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ACOUSTICS OF AUDITORIUMS
1
1 . INTRODUCTION
• Acoustics is defined as the science of sound as it deals
with origin, propagation and sensation of sound
• Sound is produced when a part of atmosphere is
compressed suddenly. Sound cannot travel in vacuum
• Unpleasant sound is called noise
• Mainly deals with reflected sound
• Here , the word auditorium means the places where
quality of sound is very important
• Ex : musical halls , seminar halls etc…
2
2 . SOUND
2.1 FREQUENCY AND INTENSITY
• Frequency is no. of pressure variations in unit time
• Intensity is flow of sound energy through unit area per time
• If I1 andI2 are intensities and they differ by n bels ,
𝑛 = log10
𝐼1
𝐼2
𝑚 𝑑𝑏 = 10 log10
𝐼1
𝐼2
The difference in loudness m is known as intensity level.
• Unit of phon indicates the level of sounds of equal loudness at
all frequencies
• The threshold of hearing is zero and that of painful hearing is
130 db
3
2.2 REFLECTION OF
• Laws of reflection
of light are
applicable
• Above assumption
is not applicable in
certain
circumstances and
great care should be
taken there
4
SOUND
• Concave surfaces lead to concentration of reflected waves
at certain points. So they are used as reflectors.
Convex surfaces spread out the waves and hence they are
used to spread the sound throughout the room.
5
2.3 DEFECTS DUE TO REFLECTED SOUND
1. ECHOES:
When reflected sound waves reach ear just when the
original sound has already been reached, an echo is produced.
• The sensation of sound persists for
1
10
th of a second
after the source has been stopped
• If the distance of reflecting surface <17m , distorted sound
will be heard
• If a no. of reflecting surfaces are provided , multiple echoes
are formed. Ex: heavy rolling sound of thunder
6
2. REVERBERATION
• Some time is needed for sound to transform to other form of
energy. This is brought about by friction b/w sound waves and air
particles as well as the surfaces against which it strikes. This
gradual process needs specific time known as reverberation time
𝑚 = 10 log10
𝐼1
𝐼2
For an average speaker ,
𝐼1
𝐼2
= 106 so that 𝑚 = 60 𝑑𝑏.
• Thus time of reverberation time is the time required by sound to
decay to one-millionth of its initial value
• Reverberation time 𝛼 𝑣𝑜𝑙𝑢𝑚𝑒 𝑜𝑓 𝑟𝑜𝑜𝑚
𝛼
1
𝑎𝑟𝑒𝑎 𝑜𝑓 ℎ𝑜𝑙𝑒𝑠 𝑖𝑛 𝑟𝑜𝑜𝑚
7
Optimum reverberation time for halls
TYPE OF HALL REVERBERATION FACTOR AUDIENCE
Churches 1.8-3 Two-thirds
Cinema theatres 1.3 Two-thirds
Music halls 1.6-2 Full
Parliament houses 1-1.5 Quorum
8
3. SABINʼS EQUATION
𝑡 =
0.16𝑉
𝐴
where t is reverberation time in seconds
V is volume in 𝑚3
𝐴 = (𝑎1𝑠1 + 𝑎2𝑠2 + ⋯)
=total absorbing power in 𝑚2- sabins .
• The unit of sound absorption (𝑚2
-sabin ) is equal to sound
absorption of one metre square area of fully open window
• If room has no holes , then A physically represents effective
area of room , as it behaves like a hole
9
4. ABSORBENT MATERIALS
Materials incorporated on the surfaces of room for better
acoustics are called Absorbent materials. Important facts
about them are:
• They should be water-proof and fire-proof
• They are soft and porous
• Their absorbing capacity depends on the thickness and
density of material and frequency of sound
• Acoustic properties can be changed by their modes of fixing
• In a big hall, audience is a major absorbing factor
• Improper covering destroys the absorbent properties of
materials
10
4.1 ABSORBENT MATERIALS
1. Hairfelt
2. Acoustic plaster
11
3. Acoustical tiles 4. Pulp boards
12
5. Compressed fibre board 6. Perforated ply wood
13
7. Wood wool board
14
5. ACOUSTIC DESIGN 0FAUDITORIUMS
1. Volume :
• The volume should be large enough such that music spreads
over the hall
• Halls of small volume are used for weak sounds
• The floor area calculated is 0.60 to 0.90 𝑚2
/person
• Average height varies between 6 m and 7.5 m
2. Site Selection :
• Mostly based on noise pollution
• If no air-conditioning is provided , orientation should be such that
external noise is limited to minimum
• Background noise level should not increase 45 𝑑𝑏
15
3. Sound absorption :
• The surface which reflects sound should be designed to assist
sound distribution
• Rear walls , balcony and concave surfaces should be provided
with absorbent materials
4. Shape :
• Convex walls are preferred over concave ones
• A fan shaped floor plan gives better performance due to
favourable reflection from sides
• For synchronisation of lip movement with sound, the distance of
farthest seat from curtain line should not exceed 23 m
16
Shapes for auditorium
17
Fan shaped plan of auditorium
18
5.Seats and seating arrangement
• The seats should be
arranged in concentric
arcs of circles
• Seats should be
provided in staggered
position
• The back to back
distance between two
rows must be at least
450 mm and maximum
limit is 1000 mm
19
Seating arrangement in auditorium
20
6. Balcony seats
• They should not be
inclined more than 300.
• If covered seats are
provided, acoustics
characteristics are not
changed considerably
• If balconies are deep ,
sound shadows may
develop
21
7. Raising and width of seats
• The successive rows
should be raised over
preceeding ones
• The rise in level varies
between 80 mm to 120
mm per row
• The width of seats
should be between 400
to 600 mm
22
5.2 DEFECTS IN AN AUDITORIUM
1. Reverberation :
• The effect of excessive reverberation is that sound once
produced prolongs for a longer duration
• The remedy is to correct time of reverberation by
installing absorbing materials
2. Loudness :
• This is due to the lack of reflecting surfaces near the
source and excessive absorption of sound in the hall
• The remedy is to provide hard reflecting surfaces near
source of sound. If length is more , more than 1 loud
speaker must be provided
23
3. Sound foci :
• In concave surfaces ,
reflected waves meet at
certain spots and create
sound of large intensity
4. Dead spots :
• Because of sound foci,
there is deficiency of
reflected sound at some
points
• This can be avoided by
providing diffusers
24
6. NOISE MAPPING
The procedure for making a
noise map or topograph is as
follows:
1. An accurate sketch
showing relative position
of all objects are drawn
2. The noise levels are
marked on suitable
number of positions
3. The connecting times
between points of equal
sound levels are drawn
and a noise map is
obtained
25
7. SOUND INSULATION
• Reduction in the level of sound when it passes through a
building component
• Hard materials are good sound insulators
• The insulation of sound is measured in adjoining room
26
OVERALL INSULATION SITUATION OF ROOMS
30 Between rooms in one house
40 Between houses,between wards in
a hospital
45 Between extra quiet wards in a
hospital
50 Between living rooms in a flat
8. CONCLUSION
• In order to attain better sound control in a room,
usually we go for acoustic materials
• We have to take each room for separate case study
and design it based on the situation prevailing
and experience of the engineer
• Sound absorption mainly deals with control of
reflected sound whereas sound proofing is
purposefully stopping the passage of sound
between two rooms
27
9. REFERENCES
1. E.G.Richardson (1957), Acoustics for Architects,
Edward Arnold (Publishers) Ltd. London
2. Fritz Ingersler (1952), Acoustics in Modern Building
Practice, The Architectural Press London
3. L.Cremer and H.A.Muller (1982), Principles and
Applications of Room Acoustics, Applied Science
4. L.Nijs and Diemer de Vries (2004), The Young
Architectʼs Guide to Room Acoustics, Acoustical
Science and Technology
5. M.Barron (1993), Auditorium acoustics and
Architectural design, E & FN Spon, London
28
6. P.Lord and D.Templeton (1986), The
Architecture of Sound; Designing Places of
Assembly, The Architectural Press, London.
7. Rangwala (2013), Building Construction,
Charotar Publishing House Pvt. Ltd. India.
8. Vern.O.Kundsen and Cyril.M.Harris (1950),
Acoustical Designing in Architecture,
Chapman and Hall, Ltd. London
29
THANK YOU
30
Any doubt????
31

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presentation

  • 2. 1 . INTRODUCTION • Acoustics is defined as the science of sound as it deals with origin, propagation and sensation of sound • Sound is produced when a part of atmosphere is compressed suddenly. Sound cannot travel in vacuum • Unpleasant sound is called noise • Mainly deals with reflected sound • Here , the word auditorium means the places where quality of sound is very important • Ex : musical halls , seminar halls etc… 2
  • 3. 2 . SOUND 2.1 FREQUENCY AND INTENSITY • Frequency is no. of pressure variations in unit time • Intensity is flow of sound energy through unit area per time • If I1 andI2 are intensities and they differ by n bels , 𝑛 = log10 𝐼1 𝐼2 𝑚 𝑑𝑏 = 10 log10 𝐼1 𝐼2 The difference in loudness m is known as intensity level. • Unit of phon indicates the level of sounds of equal loudness at all frequencies • The threshold of hearing is zero and that of painful hearing is 130 db 3
  • 4. 2.2 REFLECTION OF • Laws of reflection of light are applicable • Above assumption is not applicable in certain circumstances and great care should be taken there 4 SOUND
  • 5. • Concave surfaces lead to concentration of reflected waves at certain points. So they are used as reflectors. Convex surfaces spread out the waves and hence they are used to spread the sound throughout the room. 5
  • 6. 2.3 DEFECTS DUE TO REFLECTED SOUND 1. ECHOES: When reflected sound waves reach ear just when the original sound has already been reached, an echo is produced. • The sensation of sound persists for 1 10 th of a second after the source has been stopped • If the distance of reflecting surface <17m , distorted sound will be heard • If a no. of reflecting surfaces are provided , multiple echoes are formed. Ex: heavy rolling sound of thunder 6
  • 7. 2. REVERBERATION • Some time is needed for sound to transform to other form of energy. This is brought about by friction b/w sound waves and air particles as well as the surfaces against which it strikes. This gradual process needs specific time known as reverberation time 𝑚 = 10 log10 𝐼1 𝐼2 For an average speaker , 𝐼1 𝐼2 = 106 so that 𝑚 = 60 𝑑𝑏. • Thus time of reverberation time is the time required by sound to decay to one-millionth of its initial value • Reverberation time 𝛼 𝑣𝑜𝑙𝑢𝑚𝑒 𝑜𝑓 𝑟𝑜𝑜𝑚 𝛼 1 𝑎𝑟𝑒𝑎 𝑜𝑓 ℎ𝑜𝑙𝑒𝑠 𝑖𝑛 𝑟𝑜𝑜𝑚 7
  • 8. Optimum reverberation time for halls TYPE OF HALL REVERBERATION FACTOR AUDIENCE Churches 1.8-3 Two-thirds Cinema theatres 1.3 Two-thirds Music halls 1.6-2 Full Parliament houses 1-1.5 Quorum 8
  • 9. 3. SABINʼS EQUATION 𝑡 = 0.16𝑉 𝐴 where t is reverberation time in seconds V is volume in 𝑚3 𝐴 = (𝑎1𝑠1 + 𝑎2𝑠2 + ⋯) =total absorbing power in 𝑚2- sabins . • The unit of sound absorption (𝑚2 -sabin ) is equal to sound absorption of one metre square area of fully open window • If room has no holes , then A physically represents effective area of room , as it behaves like a hole 9
  • 10. 4. ABSORBENT MATERIALS Materials incorporated on the surfaces of room for better acoustics are called Absorbent materials. Important facts about them are: • They should be water-proof and fire-proof • They are soft and porous • Their absorbing capacity depends on the thickness and density of material and frequency of sound • Acoustic properties can be changed by their modes of fixing • In a big hall, audience is a major absorbing factor • Improper covering destroys the absorbent properties of materials 10
  • 11. 4.1 ABSORBENT MATERIALS 1. Hairfelt 2. Acoustic plaster 11
  • 12. 3. Acoustical tiles 4. Pulp boards 12
  • 13. 5. Compressed fibre board 6. Perforated ply wood 13
  • 14. 7. Wood wool board 14
  • 15. 5. ACOUSTIC DESIGN 0FAUDITORIUMS 1. Volume : • The volume should be large enough such that music spreads over the hall • Halls of small volume are used for weak sounds • The floor area calculated is 0.60 to 0.90 𝑚2 /person • Average height varies between 6 m and 7.5 m 2. Site Selection : • Mostly based on noise pollution • If no air-conditioning is provided , orientation should be such that external noise is limited to minimum • Background noise level should not increase 45 𝑑𝑏 15
  • 16. 3. Sound absorption : • The surface which reflects sound should be designed to assist sound distribution • Rear walls , balcony and concave surfaces should be provided with absorbent materials 4. Shape : • Convex walls are preferred over concave ones • A fan shaped floor plan gives better performance due to favourable reflection from sides • For synchronisation of lip movement with sound, the distance of farthest seat from curtain line should not exceed 23 m 16
  • 18. Fan shaped plan of auditorium 18
  • 19. 5.Seats and seating arrangement • The seats should be arranged in concentric arcs of circles • Seats should be provided in staggered position • The back to back distance between two rows must be at least 450 mm and maximum limit is 1000 mm 19
  • 20. Seating arrangement in auditorium 20
  • 21. 6. Balcony seats • They should not be inclined more than 300. • If covered seats are provided, acoustics characteristics are not changed considerably • If balconies are deep , sound shadows may develop 21
  • 22. 7. Raising and width of seats • The successive rows should be raised over preceeding ones • The rise in level varies between 80 mm to 120 mm per row • The width of seats should be between 400 to 600 mm 22
  • 23. 5.2 DEFECTS IN AN AUDITORIUM 1. Reverberation : • The effect of excessive reverberation is that sound once produced prolongs for a longer duration • The remedy is to correct time of reverberation by installing absorbing materials 2. Loudness : • This is due to the lack of reflecting surfaces near the source and excessive absorption of sound in the hall • The remedy is to provide hard reflecting surfaces near source of sound. If length is more , more than 1 loud speaker must be provided 23
  • 24. 3. Sound foci : • In concave surfaces , reflected waves meet at certain spots and create sound of large intensity 4. Dead spots : • Because of sound foci, there is deficiency of reflected sound at some points • This can be avoided by providing diffusers 24
  • 25. 6. NOISE MAPPING The procedure for making a noise map or topograph is as follows: 1. An accurate sketch showing relative position of all objects are drawn 2. The noise levels are marked on suitable number of positions 3. The connecting times between points of equal sound levels are drawn and a noise map is obtained 25
  • 26. 7. SOUND INSULATION • Reduction in the level of sound when it passes through a building component • Hard materials are good sound insulators • The insulation of sound is measured in adjoining room 26 OVERALL INSULATION SITUATION OF ROOMS 30 Between rooms in one house 40 Between houses,between wards in a hospital 45 Between extra quiet wards in a hospital 50 Between living rooms in a flat
  • 27. 8. CONCLUSION • In order to attain better sound control in a room, usually we go for acoustic materials • We have to take each room for separate case study and design it based on the situation prevailing and experience of the engineer • Sound absorption mainly deals with control of reflected sound whereas sound proofing is purposefully stopping the passage of sound between two rooms 27
  • 28. 9. REFERENCES 1. E.G.Richardson (1957), Acoustics for Architects, Edward Arnold (Publishers) Ltd. London 2. Fritz Ingersler (1952), Acoustics in Modern Building Practice, The Architectural Press London 3. L.Cremer and H.A.Muller (1982), Principles and Applications of Room Acoustics, Applied Science 4. L.Nijs and Diemer de Vries (2004), The Young Architectʼs Guide to Room Acoustics, Acoustical Science and Technology 5. M.Barron (1993), Auditorium acoustics and Architectural design, E & FN Spon, London 28
  • 29. 6. P.Lord and D.Templeton (1986), The Architecture of Sound; Designing Places of Assembly, The Architectural Press, London. 7. Rangwala (2013), Building Construction, Charotar Publishing House Pvt. Ltd. India. 8. Vern.O.Kundsen and Cyril.M.Harris (1950), Acoustical Designing in Architecture, Chapman and Hall, Ltd. London 29